We are given the differential equation:
\[ (t + 1) \frac{dx}{dt} = 2x + (t + 1)^4 \]
To solve this, divide both sides by \((t + 1)\):
\[ \frac{dx}{dt} = \frac{2x}{t + 1} + (t + 1)^3 \]
Now, separate the variables:
\[ \frac{dx}{2x} = \frac{1}{t + 1} dt + (t + 1)^2 dt \]
We can now integrate both sides:
\[ \int \frac{1}{2x} dx = \int \left(\frac{1}{t + 1} + (t + 1)^2\right) dt \]
The left-hand side gives:
\[ \frac{1}{2} \ln |x| \]
For the right-hand side, integrate each term:
\[ \int \frac{1}{t + 1} dt = \ln |t + 1| \quad \text{and} \quad \int (t + 1)^2 dt = \frac{(t + 1)^3}{3} \]
Thus, we have:
\[ \frac{1}{2} \ln |x| = \ln |t + 1| + \frac{(t + 1)^3}{3} + C \]
Exponentiate both sides:
\[ |x| = e^{2 \ln |t + 1| + \frac{2(t + 1)^3}{3} + 2C} \]
Simplify:
\[ x = A(t + 1)^2 e^{\frac{2(t + 1)^3}{3}} \]
Now, use the initial condition \(x(0) = 2\):
\[ x(0) = A(1)^2 e^0 = 2 \implies A = 2 \]
Thus, the solution is:
\[ x = 2(t + 1)^2 e^{\frac{2(t + 1)^3}{3}} \]
Finally, calculate \(x(1)\):
\[ x(1) = 2(1 + 1)^2 e^{\frac{2(2)^3}{3}} = 2(2)^2 e^{\frac{16}{3}} = 2 \times 4 \times e^{\frac{16}{3}} \approx 14 \]
Find \( x(1) \) given the differential equation \( (t + 1) dx = \left(2x + (t + 1)^4\right) dt \), with initial condition \( x(0) = 2 \).
This is a first order linear differential equation. The standard form is \( \frac{dx}{dt} + P(t)x = Q(t) \). The solution is found using the integrating factor method, where the integrating factor (I.F.) is \( e^{\int P(t) dt} \). The general solution is then given by \( x \cdot \text{(I.F.)} = \int Q(t) \cdot \text{(I.F.)} dt + C \).
Step 1: Rewrite the given differential equation in the standard linear form.
\[ (t + 1) dx = \left(2x + (t + 1)^4\right) dt \] \[ \frac{dx}{dt} = \frac{2x + (t + 1)^4}{t + 1} \] \[ \frac{dx}{dt} = \frac{2}{t+1}x + (t+1)^3 \] \[ \frac{dx}{dt} - \frac{2}{t+1}x = (t+1)^3 \]
This is now in the form \( \frac{dx}{dt} + P(t)x = Q(t) \), where \( P(t) = -\frac{2}{t+1} \) and \( Q(t) = (t+1)^3 \).
Step 2: Find the Integrating Factor (I.F.).
\[ \text{I.F.} = e^{\int P(t) dt} = e^{\int -\frac{2}{t+1} dt} = e^{-2 \ln|t+1|} = e^{\ln((t+1)^{-2})} = (t+1)^{-2} \]
Step 3: Multiply the standard form equation by the Integrating Factor.
\[ (t+1)^{-2} \frac{dx}{dt} - \frac{2}{(t+1)^3}x = (t+1)^3 \cdot (t+1)^{-2} \] \[ \frac{d}{dt}\left[ x \cdot (t+1)^{-2} \right] = (t+1) \]
The left side is the derivative of \( x \cdot \text{(I.F.)} \).
Step 4: Integrate both sides with respect to \( t \).
\[ \int \frac{d}{dt}\left[ x \cdot (t+1)^{-2} \right] dt = \int (t+1) dt \] \[ x \cdot (t+1)^{-2} = \frac{(t+1)^2}{2} + C \]
Where \( C \) is the constant of integration.
Step 5: Apply the initial condition \( x(0) = 2 \) to find the constant \( C \).
\[ 2 \cdot (0+1)^{-2} = \frac{(0+1)^2}{2} + C \] \[ 2 \cdot 1 = \frac{1}{2} + C \] \[ 2 - \frac{1}{2} = C \implies C = \frac{3}{2} \]
Step 6: Write the particular solution of the differential equation.
\[ x \cdot (t+1)^{-2} = \frac{(t+1)^2}{2} + \frac{3}{2} \] \[ x = (t+1)^{2} \left( \frac{(t+1)^2}{2} + \frac{3}{2} \right) \] \[ x = \frac{(t+1)^4 + 3(t+1)^2}{2} \]
Step 7: Substitute \( t = 1 \) to find \( x(1) \).
\[ x(1) = \frac{(1+1)^4 + 3(1+1)^2}{2} \] \[ x(1) = \frac{(2)^4 + 3(2)^2}{2} \] \[ x(1) = \frac{16 + 3 \cdot 4}{2} = \frac{16 + 12}{2} = \frac{28}{2} = 14 \]
Hence, the value of \( x(1) \) is 14.
Let $y=y(x)$ be the solution of the differential equation $\left(x^2-3 y^2\right) d x+3 x y d y=0, y(1)=1$.Then $6 y^2( e )$ is equal to
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,